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A NNALI DELLA

S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze

N EIL S. T RUDINGER

Remarks concerning the conformal deformation of riemannian structures on compact manifolds

Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3

e

série, tome 22, n

o

2 (1968), p. 265-274

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(2)

REMARKS CONCERNING THE CONFORMAL

DEFORMATION OF RIEMANNIAN

STRUCTURES ON COMPACT MANIFOLDS

NEIL S. TRUDINGER

(*)

§

1

Introdnction.

Yamabe

[8] seeks

to establish the

following

result:

THEOREM :

Any compact

C°° Riemannian

manifold of

dimension ~a &#x3E; 3

can be

deformned conformally

to a C°° Riemannian structure

of

constant scalar curvature.

The author has

recently

noticed that the

proof

in

[8]

appears incom-

plete, causing

the

validity

of Yamabe’s theorem to be in doubt. The pur- pose of this paper,

apart

from

indicating

this error, is to establish the re-

sult itself

under, however,

some restriction on the curvature of the manifold

(Section 3)

and also to prove a

related regularity

result for

arbitrary manifolds, naniely

that weak solutions of the deformation

problem

are

necessarily

smooth ones

(Section 4).

The

partial

results of Section 3 are sufficient to show

that,

in more

than 3

dimensions,

a structure of constant

positive

scalar curvature may be

topologically

deformed into one of constant

negative

scalar curvature.

This had

originally

been derived

by

Aubin

[1]

from Yamabe’s theorem. Ho-

pefully,

a

proof

of Yamabe’s theorem for

arbitrary compact

manifolds will be found.

We let be au n

dimensional,

C°° Riemannian

manifold, n ;:&#x3E;

3 and let gij denote its fundamental

positive

definite tensor. We consider an

arbitrary

Pervennto alla Rodazione il 28 Nov. 1967.

(*) This research was partially supported by a Ford Foundation Po8tdoctoral grant at the Conrant Institute of Mathematical Scienoed, New York University.

(3)

conformal deformation of the

writing

it as

where u

&#x3E; 0,

E C°°

(M).

_

Let

-By R

denote the scalar curvatures of the g,j

re8pectively.

Then

according

to

[8],

we have the

equation

where

denotes the

Laplace-Beltrami

i

operator corresponding

to

Thus the

problem

of

conformally deforming

the structure on M to one

of constant scalar curvature is

equivalent

to

proving

the existence of a con-

stant R and

positive,

C°°

(M)

function u

satisfying equation (2).

We take up the

study

of this

equation

in the

following

sections.

The author is

grateful

to R. Gardner and J. Moser for many useful discussions

concerning

this

problem.

§

2

Yamabe’s approach.

Yamabe

[8] considers,

instead of

equation (2),

the

equations

proving

THEOREM 1.

(Yamabe)

For any q

N,

there exists a con.3tant

~~q

and a

positive

C°°

function

uq

(normalized by f iuq Bq d v = ~ ) ( 1 ) satisfying equation (3).

M

(1) We denote the volume eletueut on M by dv and assume

(4)

267

The solutions

Âq,

7 ttq are characterized

by

the

variational problem

of

minimizing

the functional

over the class of’ functions in

W2 (2) satisfying

We denote the above class

by Aq

so that

It is

readily

seen

that 1

is

non-increasing in q

and that as q --~

~~V, iq

2013~ where

Since the

proof

in

[8]

of Theorem 1

(called

Theorem B

there)

is some-

what

unnecessarily involved,

we insert here a

simpler,

more direct version.

WTe let ,u

&#x3E;

0 denote the

ellipticity

constant of A u so that for all

points

of J.1f.

The

proof

is

split

into two

stages :

(i)

Existence in WTe choose a

« minimizing

sequence », ie a se- quence E

~4~

with as n --~ oo. Since

urn)

is bounded in

(m),

(2) The Sobolev spaces for positive integer and are defined by

and

where a~~ is a mnMi-index and is to be understood in the seiiee of distri- bution theory.

(5)

it is

weakly precompact.

We show that is in fact

precompact

in

Wl

The

argument

is a standard one in the calculus of variations

(cf. [6]). By

the Sobolev

imbedding theorem,

a

subsequence

of the

u(nJ, (which

we im-

mediately

relabel as 11(n)

itself)

converges in to a

function uq

in

A,y.

Hence for

arbitrary

E

&#x3E;

0 and

sufficiently large

m, n

depending

on t

Thus

for

sufficiently large

m, n. It then follows

(by (7))

that a«?i) converges to zcq in

lV21

We then

clearly

have

F (u,)

and hence Uq is a solution of the variational

problem.

Note that we may choose the &#x3E; 0 so that

a.e. Also the

vanishing

of the first variation

yields

the Euler-La-

grange

equations

for ’Uq, ie

for

all ~

E

1111 (M)

The function 1lq is thns a weak solution of

equation (.3).

(ii)

Sntoothne8s aoid

positivety.

We

quote

a result frome

lliptic theory.

LEMMA. Let u be a tweak

(1~1 )), non-negative,

solution in M

oj’

the

linear

equation

. where

f

E

Lr (31),

r

&#x3E; n/2.

Then u is

positive

and bounded and we the estimates

. The lemma may be

proved

in various ways. Yamabe

[8]

proves and uses

similar statements. These are also consequences of Moser’s work

(see [3],

f5],

or

[7]).

(6)

269

To

apply

the lemma to the

present situation,

we observe that u sati-

sfies a linear

equation

of form

(9)

with

where

Thus zcq is bounded and

positive. Elliptic regularity theory [2]

then guaran- tees that uq is C°°.

To establish Yamabe’s theorem from Theorem 1 it suffices to show that the functions

uq

are

equibounded

and hence

equicontinuous.

Such

is the purpose of the second

part

of Yamabe’s work

([8],

Theorem

(‘).

In

his

proof, however,

the

inequality (6.2)

appears to be in error. The correct form should be the

inequality

which is insufficient for the remainder of the

proof

to go

through.

More in-

tuitively speaking,

his

proof

of Theorem C cannot be

expected

to work since it does not

distinguish

at all two facts related to the

problem :

(i)

the presence of the term - Ru in the

equation

and

(ii)

the

compactness

of 11/.

Disregarding

these

factors,

one would not

egpect,

uniform convergence of a

subsequence

of

the Uq

but rather

merely

convergence in for

any 8 &#x3E;

0 to the trivial

solution,

as is the case with the

problem

where 92 is a bounded domain in Euclidean n-space. See

[4].

§

3 Partial

results.

We will show In the next section that a

subsequence

of

the ug

con-

verges in a certain sense to a smooth solution of

equation (2).

However the convergence is not

strong enough

to

imply

the

non-triviality

of the resul-

ting

solution. We demonstrate in this section that for a

large

class of ma-

nifolds,

the convergence is

sufficiently

nice to

guarantee

a

positive,

smooth solution of

(2).

THEOREM 2. There exists a

positive

constant 8

(depending

on

gii, R)

8itch that c, there exists cc

positive,

Coo solution

of equation (2)

with

l~ = A. Thus Yamabe’s is true under this

assumption

on the metric

gij.

(7)

PROOF. In the

equation (8)

consider a test function

The result is

and hence from

(7)

Writing

tv =

(u,)(9+1)11

the above

inequality

becomes

Let us

suppose A &#x3E;

0 and

apply

the Sobolev and Holder

inequalities.

We

obtain,

thus

since

II1tq

is bounded

independently

of q. Hence if for

large enough q

and we obtain

Clearly

from

(13),

this

inequality

continues to hold 0.

Now

choose # N -

1. Then we obtain

and

the uq

are

subsequently equibounded by

the Lemma. A

subsequence

therefore converges, with its

derivatives, uniformly

to a smooth solution of

(2),

which is also

positive by

the Lemma.

(8)

271

Note that we have the

following

bound

for ),,

and therefore the conclusion of Theorem 2 will hold if

.lt1

cial case we have then

COROLLARY 1.

Any conzpact

C°° Riemannian

1na.nifold

icith

sealar can. be

defoi-med

to a C°° Riemannian

of

constant scalar curvature.

Corollary

1 may in fact be derived very

simply

from Theorem 1. For

implies A C

0. Let the maximum value ot’ say be taken

if

on at a

point

Then since

J(P)(0

we must have

and heuce

and

accordingly

the uq are

equibounded.

Aubin

[1]

has shown that if ’It 2 3 and R is a

positive constant,

then gij may be

topologically

transformed into a metric gij with scalar curvature R

satisfying

0. Hence as a further

corollary

we have

COROLLARY 2.

If

it &#x3E;

3,

a structure

of’ positive,

constant scalfcr curva-

tui-e niay be

deforiiied topologically

into one

of

constant

negative

8calar curva.

Thus the

sign of

the tias no

topological significane

in

than t1fO

4. A

regularity

Theorem.

We prove now the

following

result

concerning

weak solutions of’ equa- tion

(

THEOREM 3. Let it be a

tt’’ (1t1)

solution

oj

an

eqttatioit of

the

(2).

Then 1i E Coo

(1lI ).

("S) The mean scalar onrvature is the quantity

(9)

PROOF. The function u satisfies

for

all ~ E j~~ {M ).

We choose

an appropriate

test

function ~ similarly

to a

method of J. Serrin

[5].

Defiue u = sup

(u, 0)

and for a

fixed fl &#x3E;

1

(to

be

eventually

chosen as in Theorem

2)

ciefine the functions

where

2q = p +

1.

-

The function G

(1t)

is a

uniformly Lipshitz

continuous function of it and hence

belongs

to Likeuise Observe also that U and F vanish for

negative

u and that

Let us now substitute in

(17)

test functions

where I

is an

arbitrary, non-negative

C

1 (M )

function. The result

is, using (7),

and hence

(10)

273

Using (19)

we then obtain

Let us

take q

now to have

compact support

in a coordinate

patch

of M.

The

integrals

in

(21)

may then be

replaced by integrals

over a

sphere S

in En of radius R

where q

= r~

(x)

E

Co (R).

We choose R so that

Then

applying

the Holder and Sobolev

inequalities

to

(21)

we obtain

and hence

We

choose fl

as in Theorem

2,

ie 1

C ~ ~ (n + 2)/(n

-

2)

so that

2q

N.

Hence we may let in

(22)

to obtain the estimate

Let

SR/2

denote the

sphere

concentric to S of radius

R/2

and choose 1] = 1 on

~2~ ! i ~~ ( c 2/R

on

SR .

Then we obtain

Replacing u by - u,

we obtain

(24)

also for the function u and

employing

a

partition

of

unity clearly provides

a

global

estimate

for some r

~&#x3E; ~

where C will also

depend

on the local

LN

norms of ~c. The boundedness of it and

subsequently

its smoothness are now conseqnences ot’ the Lemma.

Q.

F. D.

(11)

For the functions uq defined in Section

2,

we have a uniform estimate for the norms

and hence a

subsequence

converges in a weak solution of

(2).

Hence we have

COROLLARY 3. 1’he

functions

v . in

yV’_~ (ll~ ) J’or

any E

&#x3E;

0 to

a &#x3E; solution

of equation (2)

1c,ith A.

Yamabe’s tlieorein would thus follow it’ the uon

triviality

of the above solution u could be demonstrated.

This,

of course, we have

shown,

in the

preceding

section but

only

under a restriction A ~ ~ for certain

positive

c.

Added in

proof (May 1968).

Since this paper was

written,

’r. Aubin has found a

proof

of Yamabe’s theorem

by using

a

completely

different variation nal

approach.

REFERENCES

[1]

T. AUBIN. Sur la courbure scalaire des variétés riemanniennes compactes. C. R. Acad. Sci.

Paris, Vol. 262, 1966 pp. A 130-133.

[2]

L. BERS, F. JOHN and M. SCHECHTER. Partial differential equations, Part. II. New York, 1964.

[3]

J. MOSER. On Harnack’s theorem for elliptic differential equations, Comm. Pure Appl. Math., Vol. 14, 1961, pp. 577-591.

[4]

S. I. POHOZAKV. Eigenfunctions of the equation 0394u + 03BBf(u) = 0, Dokl. Akad. Nauk.

SSSR, Vol. 165, 1965 pp. 33-36.

[5] J.

SERRIN. Local behaviour of solutions of quasilinear equations, Acta Math. Vol. 113, 1965 pp. 219-240.

[6]

S. L. SOBOLEV. Some applications of functional analysis in mathematical physics, Transl.

Math. Monographs, Vol. 7, Amer. Math. Soc., Providence, R. I., 1963.

[7]

N. S. TRUDINGER. On Harnack type inequalities and their application to quasilinear ellip-

tic equations. Comm. Pure Appl. Math., Vol. 20, 1967, pp. 721-747.

[8]

H. YAMADE. On a deformation of Riemannian structures on compact manifolds. Osaka Math.

J., Vol. 12, 1960 pp. 21-37.

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